{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:47DZWCDV6EUUFPFSH5OP3JI4JD","short_pith_number":"pith:47DZWCDV","canonical_record":{"source":{"id":"1710.09956","kind":"arxiv","version":5},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-10-27T00:49:15Z","cross_cats_sorted":[],"title_canon_sha256":"0bb8adc631e486173da88231c0121b1e9511735d62d99f41210c94a1b9acd579","abstract_canon_sha256":"4741c11ae24c052b934a7c32cf42e1b8b2ee4c28315fcd37a4f2cef2e31d6ec7"},"schema_version":"1.0"},"canonical_sha256":"e7c79b0875f12942bcb23f5cfda51c48c800144dc62e75e874a47e08e73d228d","source":{"kind":"arxiv","id":"1710.09956","version":5},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1710.09956","created_at":"2026-05-18T00:12:11Z"},{"alias_kind":"arxiv_version","alias_value":"1710.09956v5","created_at":"2026-05-18T00:12:11Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1710.09956","created_at":"2026-05-18T00:12:11Z"},{"alias_kind":"pith_short_12","alias_value":"47DZWCDV6EUU","created_at":"2026-05-18T12:30:58Z"},{"alias_kind":"pith_short_16","alias_value":"47DZWCDV6EUUFPFS","created_at":"2026-05-18T12:30:58Z"},{"alias_kind":"pith_short_8","alias_value":"47DZWCDV","created_at":"2026-05-18T12:30:58Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:47DZWCDV6EUUFPFSH5OP3JI4JD","target":"record","payload":{"canonical_record":{"source":{"id":"1710.09956","kind":"arxiv","version":5},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-10-27T00:49:15Z","cross_cats_sorted":[],"title_canon_sha256":"0bb8adc631e486173da88231c0121b1e9511735d62d99f41210c94a1b9acd579","abstract_canon_sha256":"4741c11ae24c052b934a7c32cf42e1b8b2ee4c28315fcd37a4f2cef2e31d6ec7"},"schema_version":"1.0"},"canonical_sha256":"e7c79b0875f12942bcb23f5cfda51c48c800144dc62e75e874a47e08e73d228d","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:12:11.078650Z","signature_b64":"it9AvIMJ6pH1BvGlZRwyOfHoB2Amb+aiiiGAaJlttQuYc5y5rXEwgmzlwoaWfXC9xu8QuvktdfG6JLkLxBiaDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e7c79b0875f12942bcb23f5cfda51c48c800144dc62e75e874a47e08e73d228d","last_reissued_at":"2026-05-18T00:12:11.078089Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:12:11.078089Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1710.09956","source_version":5,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:12:11Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Hjw9HBz5b/s8oHpwSNET3jILk7d290wjsMvcaTTxE6b4rKFfj7kmrxdIr7RJ7tK+lHspnHNIlORXOQf3MoUgCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-07T07:31:26.521137Z"},"content_sha256":"5a8dd296893108911adada7e325876c1816b71bb5bb10039bb49e47670bed080","schema_version":"1.0","event_id":"sha256:5a8dd296893108911adada7e325876c1816b71bb5bb10039bb49e47670bed080"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:47DZWCDV6EUUFPFSH5OP3JI4JD","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Magnetic monopoles in multi-vector boson theories","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Kiyoshi Shiraishi, Koichiro Kobayashi, Nahomi Kan","submitted_at":"2017-10-27T00:49:15Z","abstract_excerpt":"A classical solution for a magnetic monopole is found in a specific multi-vector boson theory. We consider the model whose $[SU(2)]^{N+1}$ gauge group is broken by sigma-model fields (\\`a la dimensional deconstruction) and further spontaneously broken by an adjoint scalar (\\`a la triplet Higgs mechanism). In this multi-vector boson theory, we find the solution for the monopole whose mass is $M_N\\sim\\frac{4\\pi v}{g}\\sqrt{N+1}$, where $g$ is the common gauge coupling constant and $v$ is the vacuum expectation value of the triplet Higgs field, by using a variational method with the simplest set o"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1710.09956","kind":"arxiv","version":5},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:12:11Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"q8OaW2VksLcPRVa45HrY2zrjwOST8kYbyXK4T1c3Uv8x8eW3kc6IXLhFsHHUnRcqYthdvZMhv2UdcOlwV/W2CA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-07T07:31:26.521492Z"},"content_sha256":"25643f338256a1ff5e9964d4f5f1e2defbc0fc2d5094bf1b74830f09f6dedb7c","schema_version":"1.0","event_id":"sha256:25643f338256a1ff5e9964d4f5f1e2defbc0fc2d5094bf1b74830f09f6dedb7c"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/47DZWCDV6EUUFPFSH5OP3JI4JD/bundle.json","state_url":"https://pith.science/pith/47DZWCDV6EUUFPFSH5OP3JI4JD/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/47DZWCDV6EUUFPFSH5OP3JI4JD/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-06-07T07:31:26Z","links":{"resolver":"https://pith.science/pith/47DZWCDV6EUUFPFSH5OP3JI4JD","bundle":"https://pith.science/pith/47DZWCDV6EUUFPFSH5OP3JI4JD/bundle.json","state":"https://pith.science/pith/47DZWCDV6EUUFPFSH5OP3JI4JD/state.json","well_known_bundle":"https://pith.science/.well-known/pith/47DZWCDV6EUUFPFSH5OP3JI4JD/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:47DZWCDV6EUUFPFSH5OP3JI4JD","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"4741c11ae24c052b934a7c32cf42e1b8b2ee4c28315fcd37a4f2cef2e31d6ec7","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-10-27T00:49:15Z","title_canon_sha256":"0bb8adc631e486173da88231c0121b1e9511735d62d99f41210c94a1b9acd579"},"schema_version":"1.0","source":{"id":"1710.09956","kind":"arxiv","version":5}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1710.09956","created_at":"2026-05-18T00:12:11Z"},{"alias_kind":"arxiv_version","alias_value":"1710.09956v5","created_at":"2026-05-18T00:12:11Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1710.09956","created_at":"2026-05-18T00:12:11Z"},{"alias_kind":"pith_short_12","alias_value":"47DZWCDV6EUU","created_at":"2026-05-18T12:30:58Z"},{"alias_kind":"pith_short_16","alias_value":"47DZWCDV6EUUFPFS","created_at":"2026-05-18T12:30:58Z"},{"alias_kind":"pith_short_8","alias_value":"47DZWCDV","created_at":"2026-05-18T12:30:58Z"}],"graph_snapshots":[{"event_id":"sha256:25643f338256a1ff5e9964d4f5f1e2defbc0fc2d5094bf1b74830f09f6dedb7c","target":"graph","created_at":"2026-05-18T00:12:11Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"A classical solution for a magnetic monopole is found in a specific multi-vector boson theory. We consider the model whose $[SU(2)]^{N+1}$ gauge group is broken by sigma-model fields (\\`a la dimensional deconstruction) and further spontaneously broken by an adjoint scalar (\\`a la triplet Higgs mechanism). In this multi-vector boson theory, we find the solution for the monopole whose mass is $M_N\\sim\\frac{4\\pi v}{g}\\sqrt{N+1}$, where $g$ is the common gauge coupling constant and $v$ is the vacuum expectation value of the triplet Higgs field, by using a variational method with the simplest set o","authors_text":"Kiyoshi Shiraishi, Koichiro Kobayashi, Nahomi Kan","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-10-27T00:49:15Z","title":"Magnetic monopoles in multi-vector boson theories"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1710.09956","kind":"arxiv","version":5},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:5a8dd296893108911adada7e325876c1816b71bb5bb10039bb49e47670bed080","target":"record","created_at":"2026-05-18T00:12:11Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"4741c11ae24c052b934a7c32cf42e1b8b2ee4c28315fcd37a4f2cef2e31d6ec7","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-10-27T00:49:15Z","title_canon_sha256":"0bb8adc631e486173da88231c0121b1e9511735d62d99f41210c94a1b9acd579"},"schema_version":"1.0","source":{"id":"1710.09956","kind":"arxiv","version":5}},"canonical_sha256":"e7c79b0875f12942bcb23f5cfda51c48c800144dc62e75e874a47e08e73d228d","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"e7c79b0875f12942bcb23f5cfda51c48c800144dc62e75e874a47e08e73d228d","first_computed_at":"2026-05-18T00:12:11.078089Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:12:11.078089Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"it9AvIMJ6pH1BvGlZRwyOfHoB2Amb+aiiiGAaJlttQuYc5y5rXEwgmzlwoaWfXC9xu8QuvktdfG6JLkLxBiaDQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:12:11.078650Z","signed_message":"canonical_sha256_bytes"},"source_id":"1710.09956","source_kind":"arxiv","source_version":5}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:5a8dd296893108911adada7e325876c1816b71bb5bb10039bb49e47670bed080","sha256:25643f338256a1ff5e9964d4f5f1e2defbc0fc2d5094bf1b74830f09f6dedb7c"],"state_sha256":"9220ecd104a8f3492da2edc1f193624d7821cb63b80960bd804b79a79420f5e8"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"VdeW8IU6JEhq2mK8RWxHaJnWZlTAaF99ayDuBH0Iz0Nx89PVtB0MAEu25dbDcZzajL2IEp+/Vgt/NBvSiQvjAQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-07T07:31:26.523519Z","bundle_sha256":"818d807f02866f25fe2c2234d1d165e8bf2b3bd82ef091fb3cf70bf0c2f2664c"}}